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Issue
A&A
Volume 518, July-August 2010
Herschel: the first science highlights
Article Number L115
Number of page(s) 5
Section Letters
DOI https://doi.org/10.1051/0004-6361/201014638
Published online 16 July 2010
A&A 518, L115 (2010)

Herschel: the first science highlights

LETTER TO THE EDITOR

The 35Cl/$^{\sf 37}$Cl isotopic ratio in dense molecular clouds: HIFI observations of hydrogen chloride towards W3 A[*]

J. Cernicharo1 - J. R. Goicoechea1 - F. Daniel1 - M. Agúndez1,2 - E. Caux3 - T. de Graauw4 - A. De Jonge5 - D. Kester5 - H. G. Leduc6 - E. Steinmetz7 - J. Stutzki8 - J. S. Ward9

1 - Centro de Astrobiología. CSIC-INTA. Carretera de Ajalvir, Km 4, Torrejón de Ardoz. 28850, Madrid, Spain
2 - LUTH, Observatoire de Paris-Meudon, 5 Place Jules Janssen, 92190 Meudon, France
3 - Centre d'Étude Spatiale des Rayonnements, Université de Toulouse [UPS], 31062 Toulouse Cedex 9, France
4 - Atacama Large Millimeter/Submillimeter Array, ALMA Office, Santiago, Chile
5 - SRON Netherlands Institute for Space Research, Landleven 12, 9747 AD Groningen, The Netherlands
6 - Jet Propulsion Laboratory, 4800 Oak Grove Drive, MC 302-231, Pasadena, CA 91109, USA
7 - MPI für Sonnensystemforschung, 37191 Katlenburg-Lindau, Germany
8 - KOSMA, I. Physik. Institut, Universität zu Köln, Germany
9 - With Raytheon Co., Fort Wayne, Indiana, USA, since March of 2009

Received 31 March 2010 / Accepted 12 May 2010

Abstract
We report on the detection with the HIFI instrument on board the Herschel satellite of the two hydrogen chloride isotopologues, H35Cl and H37Cl, towards the massive star-forming region W3 A. The J =1-0 line of both species was observed with receiver 1b of the HIFI instrument at $\sim$625.9 and $\sim$624.9 GHz. The different hyperfine components were resolved. The observations were modeled with a non-local, non-LTE radiative transfer model that includes hyperfine line overlap and radiative pumping by dust. Both effects are found to play an important role in the emerging intensity from the different hyperfine components. The inferred H35Cl column density (a few times $\sim$1014 cm-2), and fractional abundance relative to H nuclei ($\sim$ $7.5 \times 10^{-10}$), supports an upper limit to the gas phase chlorine depletion of $\approx$200. Our best-fit model estimate of the H35Cl/H37Cl abundance ratio is $\approx$ $2.1 \pm 0.5$, slightly lower, but still compatible with the solar isotopic abundance ratio ($\approx$3.1). Since both species were observed simultaneously, this is the first accurate estimation of the [35Cl]/[37Cl] isotopic ratio in molecular clouds. Our models indicate that even for large line opacities and possible hyperfine intensity anomalies, the H35Cl and H37Cl J=1-0 integrated line-intensity ratio provides a good estimate of the 35Cl/37Cl isotopic abundance ratio.

Key words: astrochemistry - ISM: clouds - ISM: molecules - ISM: individual objects: W3 - radiative transfer - radio lines: ISM

1 Introduction

Chlorine has two stable isotopes (35Cl and 37Cl) and an ionization potential of 12.97 eV (i.e., slightly below that of hydrogen). Hence, it can be ionized by UV photons (912-956 Å) in diffuse clouds and in the edges of photon-dissociation regions (PDRs). Once ionized, Cl+ reacts with molecular hydrogen exothermically to form HCl+, a process that initiates the chemical reactions of chlorine. In cloud interiors, HCl+ can be formed by reactions starting with neutral Cl and H3+. The chemistry of chlorine in interstellar clouds has been the subject of various works (see Neufeld & Wolfire 2009). These studies predict that hydrogen chloride (HCl) is the most abundant Cl-bearing molecule in dense clouds.

The HCl hyperfine lines (see Sect. 3.2) can be resolved in interstellar sources only with heterodyne receivers equipped with high spectral resolution spectrometers. The HCl J = 1-0 line at $\sim$625.9 GHz was first detected with the Kuiper Airbone Observatory towards Orion (Blake et al. 1985) and followed by detections in Sgr B2 (Zmuidzinas et al. 1995), several positions in OMC-1 (Schilke et al. 1995), and in Mon R2 using the Caltech Submillimeter Observatory with good atmospheric transparency (Salez et al. 1996; SFL96 hereafter). The inferred HCl column densities are in the range 1013-1014 cm-2. SFL96 also presented the first detection of H37Cl towards Orion. Since the chemical reactions involving HCl are relatively well understood (see Sect. 3.2), the H35Cl/H37Cl abundance ratio should provide a good measure of the 35Cl/37Cl isotopic ratio. Both 35Cl and 37Cl nuclei are believed to form in the last burning stages of massive stars (>10 $M_\odot$) and by means of ``explosive nucleosynthesis'' during supernovae detonation (e.g., Woosley & Weaver 1995). Therefore, observations of H35Cl and H37Cl, and accurate measurements of the 35Cl/37Cl ratio in different environments, can provide some insight into the chemical evolution of both isotopes, thus into Galactic chemical evolution. The species HCl was also detected recently towards the carbon-rich evolved star IRC+10216 by Cernicharo et al. (2010).

\begin{figure} \par\rotatebox{0}{ \includegraphics[width=8.5cm]{14638fig1.eps}} \end{figure} Figure 1:

Detection of H35Cl and H37Cl J =1-0 lines towards W3 A H II region. Arrows shows the relative line strength of each HFS component. The length of the arrows are proportional to the expected intensities in the LTE optically thin limit. Both lines were observed simultaneously in a line survey of band 1b of HIFI, hence, have the same calibration accuracy. Spectral resolution was smoothed to 2 MHz ($\simeq $1 km s-1).

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Using HIFI, the Heterodyne Instrument for the Far-Infrared (de Graauw et al. 2010), on board the Herschel Space Observatory (Pilbratt et al. 2010), we present in this Letter the detection of the J=1-0 rotational transition of H35Cl and H37Cl towards the massive star-forming region W3. The broad frequency coverage of HIFI allows us to observe both isotopologues of HCl with the same relative calibration in a wide variety of astronomical environments. Here we present the first accurate determination of the 35Cl/37Cl isotopic ratio by a detailed model of the excitation of the hyperfine levels developed using a non-local radiative transfer code. The effect of line overlaps between the hyperfine components, and radiative pumping by dust photons are discussed and modeled in detail.

2 Observations and data reduction

All spectra presented here were taken during the performance verification (PV) phase of HIFI (de Graauw et al. 2010). Both H35Cl and H37Cl J=1-0 lines were observed in the Band 1b receiver using the wide band spectrometer (WBS), which provides $\sim$4 GHz of bandwidth and $\sim$1.1 MHz of channel spectral resolution (or a velocity resolution of $\sim$0.5 km s-1 at $\sim$626 GHz). The telescope, which has a half-power beam-width (HPBW) of $\sim$35''at $\sim$626 GHz, was centered on $\alpha_{2000} = 02^{\rm h}25^{\rm m}43.51^{\rm s}$, $\delta_{2000} = 62\deg 06'13''$(a position close to W3 A IRS 2 and 2a). A complete spectral scan of the Band 1b was taken at this position during PV phase and several lines from different molecules have been identified so far. The horizontal (H) and vertical (V) polarization receivers were averaged after rescaling the V one using the HCO+ J=7-6 line intensity at 624.21 GHz, i.e., close to that of HCl isotopologues. The data were first processed with HIPE software (Ott et al. 2010), and then exported to CLASS where standard data reduction routines were carried out. We checked that the target lines are not contaminated by lines from the other side band using the different frequency settings. The rms noise at $\sim$626 GHz is $\sim$30 mK (antenna temperature) per 0.5 km s-1 resolution channel. Hence, the H35Cl and H37Cl J=1-0 lines are detected at 10$\sigma$ and 6$\sigma$ levels, respectively and with the same relative calibration. At this level of sensitivity, only the most abundant species are detected. In particular, we detected 20 lines in the entire band 1b above 3$\sigma$. The brightest is the CO J=5-4 line, followed by the ground-state line of ortho-H2O and a few lines from formaldehyde, methanol, HCO+, and HCN. Hence, we are confident that the observed HCl line profiles are not blended with other spectral features. By examining our own and public spectral catalogs (Pickett et al. 1998; Muller et al. 2001,2005), we also checked that lines in the signal band from other molecules do not blend with the hyperfine components of both HCl isotopologues.

The total integration time was 2 min. Figures 1 and 2 show the resulting line profiles (data smoothed to a spectral resolution of $\simeq $1 km s-1). To compare with our models, the following expression for the main beam efficiency was adopted, $\eta_{\rm mb} = 0.72~\exp(-(\nu/6)^2)\times0.96$, where $\nu$ is the frequency in THz, 0.72 is $\eta_{\rm mb}$ for the telescope in the limit of 0 frequency, and the factor 0.96 is the assumed forward efficiency of the telescope (Olberg priv. comm.).

3 Results

In terms of spectroscopy, the I=3/2 nuclear spin of 35Cl and of 37Cl splits the pure rotational transitions of H35Cl and H37Cl into several hyperfine structure (HFS) components (see e.g., Cazzoli & Puzzarini 2004 and references therein). These hyperfine components are indicated as vertical arrows in Fig. 1. In the optically thin limit, these components follow a 2:3:1 intensity ratio (from the lowest to the highest frequency hyperfine component). It is clear from Fig. 1 that the observed ratios are close to 1:1:1 for the three hyperfine components of H35Cl. These ratios indicate that the H35Cl hyperfine components are affected substantialy by opacity. Even for H37Cl, the observed hyperfine line intensities (1:1:2) do not follow the expected ratios in an optically thin case.

\begin{figure} \par\rotatebox{0}{ \includegraphics[width=8.5cm]{14638fig2.eps}} \end{figure} Figure 2:

H35Cl, H37Cl J=1-0, and C17O J=5-4 lines observed with HIFI towards W3 A. Continuous curves show closest fitting radiative-transfer model line profiles (see text). The spectral resolution is $\simeq $1 km s-1.

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The intensity peak ratio of the strongest H35Cl and H37Cl HFS components is $\simeq $1.5 and the integrated intensity ratio is $\simeq $$2 \pm 0.2$. These values are lower than the solar 35Cl/37Cl abundance ratio, $\sim$3.1 (Anders & Grevesse 1989), which suggests that optical depth effects could influence the observed HFS line intensity ratios (or that the H35Cl/H37Cl abundance ratio is lower than the solar value). For completeness, Fig. 2 compares the detected HCl lines with the C17O J = 5-4 at 561.712 GHz also observed with HIFI. The detection of C17O, HCO+ and HCN mid-J lines confirms the presence of warm and dense molecular gas towards the observed position.

3.1 HCl excitation and $^{\sf 35}$Cl/$^{\sf 37}$Cl abundance ratio

The star-forming region W3 is located in the Perseus arm at a distance of 2.3 kpc and contains several young massive stars that ionize a natal molecular cloud creating H II regions. In particular, the near-IR sources IRS 2 and IRS 2a (OB stars) are believed to be the ionizing sources of the W3 A H II region (Tieftrunk et al. 1995 and references therein). These sources are also the origin of molecular outflows and are X-rays emitters (Hofner et al. 2002).

\begin{figure} \par { \includegraphics[angle=-90,width=8.5cm]{14638fig3.eps} }\end{figure} Figure 3:

Results from non-local, non-LTE radiative transfer calculations for the H35Cl J=1-0 HFS components. The different curves show the effects of including line overlap and radiative pumping from dust photons in the emerging line intensities and relative HFS line ratios.

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To estimate the H35Cl/H37Cl abundance ratio and analyze all possible effects affecting the emerging line profiles, we modeled the observed HCl and C17O lines with our non-local and non-LTE radiative transfer codes (González-Alfonso & Cernicharo 1993; Daniel & Cernicharo 2008; Goicoechea et al. 2006; González-Alfonso & Cernicharo 1997). To take into account the blending of the HCl J =1-0 hyperfine components (i.e., to determine the opacity at each frequency when several lines overlap), we used the modelling approach presented in Daniel & Cernicharo (2008) to interpret the HFS line emission from N2H+, HCN, and HNC. Rate coefficients for the collisional excitation of HCl by He are taken from Neufeld & Green (1994), who also estimated the contribution to each specific hyperfine level.this volume Like other light hydrides that HIFI will observe, HCl has a large rotational constant (10.4 cm-1), thus HCl rotational transitions have high spontaneous radiative rates. The HCl critical densities are very high, $n_{\rm cr}$(J=1-0)  $\simeq 7 \times 10^7$ cm-3, and only when n(H2)  $\gtrsim~n_{\rm cr}$ does collisional excitation dominate. This high value suggests that HCl line emission arises in dense molecular gas. Radiative pumping by dust photons may also be very important in determining the HCl level populations (see also SFL96) because of the increase in grain emissivity and dust opacity in the far-IR and submillimeter domains (Cernicharo et al. 2006a,b). Model predictions shown in Fig. 3 demonstrate that the inclusion of line overlap, dust pumping, and both effects together, modifies the relative intensity of each HFS component. We note in particular how the J=1-0 F =1/2-1/2 line (the HFS component with the weakest line strength and opacity) is enhanced with respect to the other components when radiative pumping is included.

To reproduce the observed H35Cl and H37Cl line profiles and relative intensities, we assumed uniform physical conditions ( $n_{\rm H} \simeq 10^6$ cm-3 and $T_{\rm k} \simeq 100$ K; taken from Helmich et al. 1994; Tieftrunk et al. 1995) and that the H35Cl and H37Cl abundances are free parameters. The C17O line was also analyzed with the same parameters to verify the model consistency. In particular, the C17O J=5-4 line was found to be optically thin ( $\tau \simeq 0.1$), which allowed us to constrain the line-of-sight column density of material and also the line velocity dispersion ( $\sigma \simeq 1.3$ km s-1). Gas and dust were assumed to coexist and be thermally coupled ( $T_{\rm k} = T _{\rm d}$).

To reproduce the observed HCl line peak positions and their relative strengths, best fit solutions were obtained for an expanding shell of gas. The adopted velocity gradient (from 2.5 km s-1 at the center to 0.5 km s-1 at the edge) is consistent with the CO molecular outflows seen in the region (e.g., Hasegawa et al. 1994). Optimal results were obtained for a H35Cl column density of a few times 1014 cm-2 (or an abundance of $\sim$ $7.5 \times 10^{-10}$ relative to total H). The inclusion of radiative pumping from dust (and line overlap to a lesser extent) allowed one to more accurately reproduce the observed HFS relative line intensities. Assuming that H35Cl and C17O arise from the same regions, we inferred a column density ratio of N(H35Cl) $\simeq $ N(C17O)/20, by using the CO abundance determined for the region ($\sim$ $4 \times 10^{-5}$ per H nucleus; Tielens et al. 1991) and assume a standard 16O/17O isotopic ratio of 2600. Optimal fits were obtained by using an automatic $\chi^2$procedure and are shown in Fig. 2. The H35Cl/H37Cl abundance ratio found in the models is $\sim$2.1 (with a confidence interval within 1.6-3.1). Since H35Cl lines are moderately optically thick ( $\tau \sim 12$, 8, 4 for each HFS component), one does not expect the observed H35Cl/H37Cl line intensity ratio to provide a direct measure of the H35Cl/H37Cl abundance ratio. However, HCl critical densities are much higher than the gas density in most ISM clouds, and therefore the excitation temperature of the different HFS components remain proportional to the HCl column density, even for optically thick lines. To conclude whether or not the line integrated intensity ratio is a good measure of the isotopic abundance ratio, Fig. 4 shows the modeled integrated intensity ratio as a function of the H35Cl/H37Cl abundance ratio. Although the hyperfine components are optically thick in most models, the integrated line intensity ratio is proportional to the isotopic ratio for HCl abundances below 10-9. In Fig. 4, we also show the results for a static cloud. In this case, the opacities are larger but the integrated intensity ratio still provides a reliable measurement of the isotopic abundance ratio for HCl abundances below 10-10.

\begin{figure} \par\includegraphics[angle=-90,width=8.5cm]{14638fig4.eps} \end{figure} Figure 4:

Modeled HCl and H37Cl J=1-0 integrated line intensity ratio (R) as a function of the assumed isotopic abundance ratio (see text). HCl abundances, indicated at the top left, are relative to H nuclei. Continuous lines correspond to models with a velocity gradient. Dashed lines correspond to a static model.

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\begin{figure} \par\includegraphics[angle=-90,width=8.5cm]{14638fig5.eps} \end{figure} Figure 5:

Cloud-depth dependent photochemical models adapted to W3 A physical conditions. The gas density ( $n_{\rm H} =10^6$ cm-3) and temperature (Tk =100 K) are kept constant. The UV radiation field is $\chi =10^4$ and the ionization rate due to cosmic rays is $\zeta $(H) =  $2.5 \times 10^{-17}$ s-1. The predicted abundance of several Cl-bearing species are shown. A chlorine gas-phase abundance of $1 \times 10^{-9}$ is used. The dashed line shows the expected HCl abundance with an undepleted abundance of [Cl] =  $1.8 \times 10^{-7}$.

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3.2 Chlorine chemistry in W3 A H9pt11ptII region

In the UV-illuminated gas, the chlorine chemistry involves the reaction of Cl+ with molecular hydrogen to form HCl+, which then reacts with H2 to produce H2Cl+. If the abundance of electrons is high, dissociative recombination of H2Cl+ leads to the formation of HCl with a typically assumed branching ratio of $\sim$10%. In cloud interiors, atomic chlorine is mostly neutral, not ionized, so that the reaction of Cl and H3+ drives the formation of H2Cl+, which then reacts with CO and H2O leading to the formation of HCl. An alternative direct route to HCl in either hot gas or regions where vibrationally excited H2 is abundant (e.g., Agúndez et al. 2010) is the Cl + H2  $\rightarrow$ HCl + H reaction, which possesses an energy barrier of $\sim$0.2 eV (Dobis & Benson 2002). The destruction of HCl is dominated both by photoionization and photodissociation and by reactions with C+ and H3+ (the latter in the UV shielded gas). Previous observational studies of HCl suggest that there has been a depletion of gas-phase chlorine in dense molecular clouds of a factor of >100 (SFL96) relative to the elemental chlorine abundance observed in diffuse clouds ([Cl]$\simeq $ $1.8 \times 10^{-7}$; Savage & Sembach 1996, Sonnentrucker et al. 2006 and references therein). To follow the HCl chemistry in the particular environment of W3 A H II region and estimate the Cl depletion we modeled the Cl-photochemistry using the Meudon PDR code (Le Petit et al. 2006; Goicoechea & Le Bourlot 2007). The reaction network for Cl-bearing molecules includes the updated rates of Neufeld & Wolfire (2009). We note that the X-ray luminosity reported in the region ( $L_{\rm X} \sim 5 \times 10^{31}$ erg s-1; Hofner et al. 2002) is insufficient for a ``XDR-'' rather than a ``PDR-dominated'' environment. However, in cloud interiors X-ray photons may play an important role in the Cl-chemistry.

Figure 5 shows the output of a model adapted to the physical conditions in W3 A. The UV radiation field producedthis volume by the OB stars in the region is simulated by an enhancement of 104 times the mean interstellar radiation field (in Draine units). To reproduce the inferred H35Cl abundance ($\sim$ $7.5 \times 10^{-10}$), a gas-phase chlorine depletion of $\lesssim$200 is needed, HCl accounting for $\approx$70% of the Cl nuclei in the gas phase. This conclusion is reached assuming that the observed HCl arises in regions of large H2 column density ( $A _{\rm V} \gtrsim 100$; see Sect. 3.1), which is consistent with the submm continuum maps of the region (Jaffe et al. 1983). If the observed HCl arises in regions of lower extinction, the Cl depletion factor will obviously be lower.

4 Conclusions

We have presented the first detection of H35Cl and H37Cl towards the W3 A H II region. The inferred H35Cl column density (a few times $\sim$1014 cm-2) and fractional abundance ($\sim$ $7.5 \times 10^{-10}$ per H nucleus) provide an upper limit to the gas phase chlorinedepletion of $\approx$200. This value is lower than that observed towards Orion hot core, but similar to that inferred towards Mon R2 (SFL96). Radiative transfer models including HFS line overlap and pumping by dust photons have been used to interpret the observations. The best-fit model provides a H35Cl/H37Cl abundance ratio of $\approx$2.1, which is both lower than the solar value ($\approx$3.1) and lower than the previous estimate towards Orion ($\approx$4-6; SFL96). On the other hand, it is similar to the [35Cl]/[37Cl] ratio obtained in the IRC+10216 circumstellar envelope from [Na35Cl]/[Na37Cl] and [Al35Cl]/[Al37Cl] measurements (Cernicharo et al. 2000; Cernicharo & Guelin 1987).

Acknowledgements
HIFI has been designed and built by a consortium of institutes and university departments from across Europe, Canada and the United States under the leadership of SRON Netherlands Institute for Space Research, Groningen, The Netherlands and with major contributions from Germany, France and the US. Consortium members are: Canada: CSA, U.Waterloo; France: CESR, LAB, LERMA, IRAM; Germany: KOSMA, MPIfR, MPS; Ireland, NUI Maynooth; Italy: ASI, IFSI-INAF, Osservatorio Astrofisico di Arcetri- INAF; Netherlands: SRON, TUD; Poland: CAMK, CBK; Spain: Observatorio Astronómico Nacional (IGN), Centro de Astrobiología (CSIC-INTA). Sweden: Chalmers University of Technology - MC2, RSS & GARD; Onsala Space Observatory; Swedish National Space Board, Stockholm University - Stockholm Observatory; Switzerland: ETH Zurich, FHNW; USA: Caltech, JPL, NHSC. We thank the Spanish MICINN for funding support through grants AYA2006-14876, AYA2009-07304, and and Consolider project CSD2009-00038. J.R.G. is supported by a Ramón y Cajal research contract from the Spanish MICINN. MA is supported by a Marie Curie Intra-European Individual Fellowship within the EC FP7 under grant agreement no 235753.

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Footnotes

... W3 A[*]
Herschel is an ESA space observatory with science instruments provided by European-led Principal Investigator consortia and with important particiation from NASA.

All Figures

  \begin{figure} \par\rotatebox{0}{ \includegraphics[width=8.5cm]{14638fig1.eps}} \end{figure} Figure 1:

Detection of H35Cl and H37Cl J =1-0 lines towards W3 A H II region. Arrows shows the relative line strength of each HFS component. The length of the arrows are proportional to the expected intensities in the LTE optically thin limit. Both lines were observed simultaneously in a line survey of band 1b of HIFI, hence, have the same calibration accuracy. Spectral resolution was smoothed to 2 MHz ($\simeq $1 km s-1).

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In the text

  \begin{figure} \par\rotatebox{0}{ \includegraphics[width=8.5cm]{14638fig2.eps}} \end{figure} Figure 2:

H35Cl, H37Cl J=1-0, and C17O J=5-4 lines observed with HIFI towards W3 A. Continuous curves show closest fitting radiative-transfer model line profiles (see text). The spectral resolution is $\simeq $1 km s-1.

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In the text

  \begin{figure} \par { \includegraphics[angle=-90,width=8.5cm]{14638fig3.eps} }\end{figure} Figure 3:

Results from non-local, non-LTE radiative transfer calculations for the H35Cl J=1-0 HFS components. The different curves show the effects of including line overlap and radiative pumping from dust photons in the emerging line intensities and relative HFS line ratios.

Open with DEXTER
In the text

  \begin{figure} \par\includegraphics[angle=-90,width=8.5cm]{14638fig4.eps} \end{figure} Figure 4:

Modeled HCl and H37Cl J=1-0 integrated line intensity ratio (R) as a function of the assumed isotopic abundance ratio (see text). HCl abundances, indicated at the top left, are relative to H nuclei. Continuous lines correspond to models with a velocity gradient. Dashed lines correspond to a static model.

Open with DEXTER
In the text

  \begin{figure} \par\includegraphics[angle=-90,width=8.5cm]{14638fig5.eps} \end{figure} Figure 5:

Cloud-depth dependent photochemical models adapted to W3 A physical conditions. The gas density ( $n_{\rm H} =10^6$ cm-3) and temperature (Tk =100 K) are kept constant. The UV radiation field is $\chi =10^4$ and the ionization rate due to cosmic rays is $\zeta $(H) =  $2.5 \times 10^{-17}$ s-1. The predicted abundance of several Cl-bearing species are shown. A chlorine gas-phase abundance of $1 \times 10^{-9}$ is used. The dashed line shows the expected HCl abundance with an undepleted abundance of [Cl] =  $1.8 \times 10^{-7}$.

Open with DEXTER
In the text

Copyright ESO 2010

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